Electro-optical apparatus



July 15, 1941. F. GRAY ELECTRO-CPTICAL APPARATUS Original Filed March 4, 1936 2 Sheets-Sheet l m. s Q

/NvfNroR 5y F. GRAY ATTORNEY July 15, 1941. F. GRAY ELECTRO-OPTICAL APPARATUS Original Filed March 4. 1936. 2. Sheets-Sheet 2 TOR A7" ORNEV Patented July 15, 1941 ELECTRO-OPTICAL APPARATUS Frank Gray, New York, N. Y., assigner to Bell 1 Telephone Laboratories, Incorporated, New

York, N. Y., a corporation of New York Original application March 4, 1936, Serial No. 67,059. Divided and this application August 25, 1938, Serial No. 226,633

(Cl. Z50-153) y mesh electrode adjacent the coating of photo- 13 Claims.

This invention relates to electro-optical apparatus and more particularly to means for setting up electric currents representative of the various light-tone values of an object, as in television scanning.

Certain light sensitive electric materials will have a large response to light of wave-lengths Within a certain range and zero or negligibly small response in another range or ranges. It has been discovered that this phenomenon can be put to use in electro-optical systems, as for example, television transmission systems, so that a light sensitive electric image receiving plate or layer may be associated with a second light sensitive electric layer adapted to -be scanned by a beam of light to produce image currents dependent upon the light intensities oi the elemental areas of the image plate, the material of one or both layers being chosen with regard to the wave-length range of sensitivity, and the Wavelengths of either the scanning beam or the image light beam, or both, also being chosen so that one or the other of these beams may pass through one layer :to the other without aiIecting it, or each beam may impinge upon both layers while affecting only one, or each beam may impinge upon a diieren-t layer, thus each beam affecting only one.

An object of this invention is to provide apparatus for utilizing the phenomenon mentioned above in the production of electric currents under control of light.

Another object is to provide novel means for producing image currents for use in systems of television and telephotography.

A further object of this invention is to provide scanning apparatus which, while not utilizing the phenomenon mentioned above,4 provides means for making each film or layer responsive to a different beam of light.

In accordance with one embodiment of the invention, chosen for purposes of illustration and hereinafter described in detail, a gas-tight container encloses a target. comprising a metallic plate carrying a photo-conducting fllm, i. e., a film formed of material adapted to have its conductivity increased when supplied with radiations of a wave-length range to which it is sensitive, which range will be designated the first range, on which is applied a very thin illm or coating of a non-conducting photo-emissive material adapted to emit electrons when exposed to radiations oi a second wave-length range which radiations, however, do not aect the conductivity of the photo-conducting illm, and a ne emisslve material. Associated with the container is a means for applying radiations of the first wave-length range to an object and for directing radiations reiiected from the object, through the interstices of the mesh electrode and the photo emissive layer. upon the photo-conducting lm to control its conductivity. Also associated with the container is a means for producing a moving beam of radiations of the second wave-length range and for causing it to pass through the interstices of the electrode to scan successively the elemental areas of .the photo-emissive ycoating. which is thereby activated to cause the production of a moving beam o1 electrons which passes to the mesh electrode, to thereby cause a flow of image current .to an external circuit. The ilow of photo-electrons from an elemental area of the photo-emissive coating is controlled by the conductivity imparted to successive elemental areas of the underlying photo-conducting layer by radiations corresponding to the lights and shades of the object.

As an alternative, radiations reflected from the object may be applied to the photo-emissive coating from a range which cause it to emit electrons but which do not aiect the conductivity of the photo-conducting illm and an image current may be produced by scanning the photo-conducting lm with a beam oi radiations which renders its elemental areas conductive in turn but which does not cause the photo-emissive coating to emit electrons.

In another embodiment, the target may comprise a metal plate, a pair ot photo-conducting illms of materials respectively sensitive to difierent wave-length ranges of radiations, and a transparent conductive layer. Radiations oi one wave-length range reflected from the object control the conductivity of the elemental areas of one of the illms in accordance with the light-tone values of the corresponding elemental areas ot the object while a beam of radiations of a second wave-length range scans in succession the elemental areas of the second lm through the transparent layer and the ilrst film to successively render these elemental areas conducting. The external circuit is connected to the metal plate and .the transparent conductive layer, so that when the elemental areas of both films are made conducting by the radiations projected on them respectively, an image current which varies with the light tone values of the object passes through this external circuit.

As an alternative to this embodiment, the target may 'comprise a transparent plate provided with a transparent metal coating carrying two superposed iilms of photo-conducting material and a transparent conducting layer, 4the image controlled radiations being applied to one film from a position in iront of the target to control the conductivity applied to its respective unit areas, as described above, while the scanning beam of radiations of a different wave-length range is directed through the transparent plate to the other iilm from. a position behind the target. The external circuit is connected between the metal coating and the conducting layer and an image current is supplied to that circuit in a manner similar to that described above. The target may be applied to the external surface of the end wall of a cathode ray tube, i. e., the wall carrying the fluorescent screen, and radiations from the fluorescent spot may be'used to eiiect scanning. Again, the target may comprise two photo-conducting iilms of the; same material separated -by an intervening black. high resistance layer, which prevents the scanning spot from affecting the photo-conducting nlm to which the image controlled radiations are applied. As a further alternative, a single film of photo-conducting material may be used, provided it is just thick enough to prevent the scanning spot and the radiations controlled by the object from affecting it throughout. In either of the two last-mentioned alternatives, radiations of the same type may be used both for illuminating the object and for scanning the target.

If the photo-conducting layers in any of the above embodiments are made of a material having high specific resistance and are made relatively thin compared to the size of the area covered by the scanning light beam, they may be made continuous as the lateral conductivity therethrough will be so small as to be negligible. The thin film and the high speciiic resistance help to produce a large stored charge which is discharged by the scanning beam.

The invention will be more readily understood by referring to the following description, taken in connection with the accompanying drawings forming a part thereof, in which:

Fig. 1 is a diagrammatic representation of a television system including the invention;

Fig. 2 is an enlarged perspective view of the assembly used in the scanning tube of Fig. l:

Fig. 3 is an enlarged perspective view of a type of assembly that may be used as an alternative to that shown in Fig. 2:

Fig. 4 shows a system somewhat similar to that of Fig. 1 embodying a modiiied method of scanning;

Fig. 5 is an enlarged perspective view of the assembly used in the scanning tube of Fig. 4;

Fig. 6 shows an image target mounted on the end of a cathode ray tube; and

' Figs. 7 and 8 are modifications of the arrangement shown in Fig. 8.

Referring more particularly to the drawings, Fig. 1 shows a television system which, in general, comprises a television transmitter T connected by a transmission channel L to a television receiver R.

The transmitter T includes a scanning tube S, an optical system ll for gathering radiations of one type, reflected from an object O, and for directing these radiations to a target included in the scanning tube, and means, such as the cathode ray tube C, for producing a moving beam of radiations oi a second type and, in cooperation with a suitable optical system 2|, for causingthisbeamtoscanthetarget. Scanningtube S comprises a gas-tight container I0 of glass or other suitable material enclosing an image target or screen, represented generally as ll, and a line mesh electrode i2 spaced therefrom.

In order to clarify the detailed description of the system of Fig. 1, reference will now be made to Fig. 2, which illustrates an enlarged perspective view of the assembly used in the scanning tube S, with the glass container broken away. As therein shown, the assembly comprises a suitable anode, such as the mesh electrode I2, and a target or screen Il comprising in order (starting from the side remote from the electrode l2): a metal plate Il carrying a photoconducting nlm I4 which in turn carries a comting I5 of photo-emissive material. 'Ihe conductivity of the photo-conducting film I4 increases when supplied with radiations of one wave-length range, which for convenience will be hereinafter designated A-radiations, while the photo-emissive coating II is sensitive to a second wave-length range of radiations, hereinafter designated B-radiations, which do not aiiect the conductivity of the nlm I4.

'I'he fine mesh electrode l2 is adjacent the photo-emissive coating I5 and is connected to the metal plate il by an external circuit, including a battery I6 and a resistance l1, the latter being included in the input circuit of an amplifier i8. 'I'he negative terminal of the battery Il is connected to the metal plate I3 and the battery's positive terminal is connected to the mesh electrode l2 through the resistance I1, whereby this electrode is polarized to operate as an anode with respect to the plate il.

The object or neld oi view O is supplied with radiations from a suitable source, not shown, and these radiations are reilected from the object through an optical system, represented generally by thelens Il, through the interstices of the mesh electrode I2 and through the thin coating I5 onto the photo-conducting nlm I4 where an image of the object O in A-radiations is formed. The small areas of the film Il are thereby successively rendered conducting in accordance with the tone values of the corresponding small areas of the image iield O. A suitable optical filter 20 may be inserted between the object O and the lens II in order to pass `only the type of radiations desired.

Also associated with the scanning device S is a second optical system represented by a means for generating a moving spot of light and a lens system, represented generally by a lens 2l, for

forming a moving beam of radiations to scan the surface of the photo-emissive coating li. The means for generating the moving spot of light is represented, and will be described more fully below, as a cathode ray tube C having a iluorescent screen 22, but any other suitable type of apparatus for producing this result may be used, as for example. a source of radiations associated with a disc having a series of apertures arranged in a spiral. y

The cathode beam of the tube C is deflected in two directions at right angles to each other and at such relative speeds in the two directions that the screen 22 is excited to iiuorescence to produce a moving spot of radiations which covers the entire screen in a time interval within the period oi' persistence of vision, in order to prevent iiicker. Deiiectlon of the beam in one di- 'tions increase the conductivity of rection is effected by the field between a pair of deflecting plates 23 supplied with current having a saw-toothed wave form, the production of this current being controlled by oscillations oi' line scanning frequency supplied by the oscillator 24 to the deflecting-current producing device 25. Deilection in the other direction is produced by supplying a second pair of' deilecting plates 26 with a current, also oi' saw-tooth wave form, supplied by the deflecting-current producing device 21, controlled by oscillations of image cycle frequency produced by a subharmonic generator 28 supplied with oscillations from the oscillator 24. Any suitable apparatus, such as that disclosed in United States Patent 1,613,954, January 11, 1927, to Knoop, may be used to produce the deflecting currents.

'Ihe operation of the scanning tube S is as follows:

A-radiations from a suitable source (not shown) are reflected by the object O and proiected through the interstices of the mesh electrode I 2 and the photo-emissive coating I5 upon the photo-conducting illm I4. 'Ihese A-radiathe film I4 but do not produce any emission from the layer I5. A beam of radiations from the moving spot of light produced by the fluorescent screen 22 is directed by the lens system 2| through the interstices of the mesh electrode cessively the elemental areas of the photo-emisslve coating I5. 'I'hese radiations are of the second, or B-type, and cause the coating I to be activated to cause the flow of a moving beam of photoelectrons to the mesh electrode I2, the flow from any elemental area being controlled by the conductivity imparted to the corresponding elemental area of the photo-conducting film I4 by the radiations reflected by the object O. In other words, the resistance of the circuit through the tube at any instant is dependent upon the resistance of the elemental area of the photoconducting film I4 which corresponds to the elemental areas of the photo-emissive coating I5 being scanned at that time. The resistance of the elemental areas of the film I4 is determined by the intensity of the radiations reflected from the object O onto the successive elemental areas of the film. Thus, an image current varying with the tone values of successive elemental areas of the image O is caused to flow through the external circuit including the resistance I1, as described above, when it is supplied, after amplification by the device I8, to a transmission circuit and over a line L, or a line carrier or radio channel, to a distant receiving station which includes a receiver R.

Receiver R may include an amplifier, in case the image current is directly transmitted, or a demodulator and amplifier in case transmission is effected in accordance with line carrier or radio practice. It may also include a cathode ray discharge device 30 comprising a cathode 3| and an anode 32 for producing the cathode beam, two pairs of plates 33 and 34 for respectively effecting deflection of the beam in two directions at right angles to each other, a fluorescent screen 35, and a pair of control grids 36 and 31 connected by an external circuit 38 to which the image currents received over line L and amplified by the device 39 are supplied by means of a transformer 40. Auxiliary devices 4I, 42 and 43, similar to those described in connection with I2 to scan sucthe transmitter, are also used in the receiving system R. Devices 4I and 42 operate, as disclosed in the Knoop patent, to supply deflecting current of saw-tooth wave form to respective pairs of deflecting plates 34 and 33. The apparatus for producing the deflecting current is controlled by current of line scanning frequency received from the oscillator 24 via a transmission line or radio channel, which has not been shown. but its feeders have been designated as L and L". In this manner, the cathode beam of the receiver R is deflected in synchronism and in phase with the deflection oi the cathode ray beam of the discharge device C used at the transmitter.

The cathode ray discharge device 30 at the receiving station operates in the following manner:

The control electrodes or grids 36 and 31 are closely adjacent each other in a position between the anode 32 and the fluorescent screen 35 and comprise segments of a sphere, the centers of which are close to the centers of the deflecting fields produced by the pairs of plates 33 and 34. The grid 36 is maintained at substantially the same potential as the anode 32 and the signal potentials are applied to the grid 31, which may be negatively polarized with respect to the grid 36. The two grids, therefore, serve to define a very limited zone in which the signal potentials are effective for controlling the cathode beam, and this zone is substantially isolated from the equipotential section established between the anode 32 and the grid 36, within which zone deflection of the beam is effective. Consequently, deflection of the beam is controlled by the fields established between the pairs of plates 33 and 34 without being influenced by the signal potentials, and the signal potentials operate to control the velocity or number of electrons constituting the beam and hence the intensity of the excitation of the fluorescent screen, which determines the quality of the image produced, without causing the direction of travel of the electrons to be varied. In other words, the two sets of elements for effectively controlling the deflection and in- April 18, 1939, to J. B. Johnson. While a receiver of the cathode ray discharge type has been described, it will, of course, be obvious that a glow lamp cooperating with a revolving disc having a spiral of apertures, or any other well-known receiver may be used with my invention. A satisfactory receiver of the glow lamp type is disclosed in United States Patent 1,728,122, September 10,` 1929, to Horton.

The A-radiations may be red or infra-red, or in other Words, those radiations having a wavelength greater than about 6500 Angstrom units, while the B-radiations may be blue, violet, or ultra-violet, or in other words, those radiations having a wave-length less than about 4700 Angstrom units. 'I'he wave-lengths given above are merely by way of example and this invention is not specifically limited thereto. While in Fig. 1 a system has been described in which the object has applied thereto A-radiations while the scanning beam is of B-radiations, it is to -be understood that B-radiations may be used to reflect an image of the object onto the photo-emissive coating Ii, whereby it is actuatedto cause the emission of electrons, these B-radiations not af- Iecting the conductivity oi the photo-conducting nlm Il; and the illm I4 may be scanned with a beam of A-radiations whichaiiects its conductivity but which does not cause electronic emission from the layer It. The scanning beam in this arrangement renders the elemental areas oi the illm il successively conductive as they are scanned in turn.

The cathode ray tube is well suited Ior use as a source for supplying a scanning beam o! B- radations as the spot ot light given oi! by the fluorescent screen is rich in radiations in the e blue, violet and ultra-violet portions oi the spectrum. II ultra-violet radiations are used for the scanning beam, the lens in the optical system 2l as well as the material oi the enclosure should be of a suitable substance to pass the radiations such as, for example, quartz. Also, it might be desirable in some cases to include within the optical system represented by 2| a suitable optical filter to filter out all undesired radiations.

The assembly shown in Fig. 2 may comprise a iilm Il of selenium or other suitable material made oi discrete particles so that the lateral conductlvity is negligibly small. IThe film may be in globular form. Selenium is particularly sensitive to red and infra-red radiations. The very thin, and hence, discontinuous transparent, photo-emisslve coating I5 may be made of a suitable alkali metal sensitive to blue, violet, or ultraviolet radiations, such as for example, potassium hydride. The film I4 may comprise a thin. continuous illm which may have its lateral conductivity decreased by cross-hatching the nlm with fine lines through to the metal plate il, or the surface of the metal plate may be cross-hatched with numerous, deep, and narrow grooves.

The operation described above may be called the "resistance method. If the thin illm I4 is of sufiiciently high speciiic resistance, the device will operate by another method, that is, by the so-called storage method because charges are laid down on one surface or the photo-conducting element which leak ofi during the next image cycle, the recharging current thus forming a greatly increased image current. This high specinc resistance also makes possible the use of a continuous film oi photo-conducting material while still restraining the lateral conductivity to a negligible minimum, provided that the thickness of the film is small compared to the diameter of the scanning spot, that is, for example. one-tenth of that diameter. For a more complete description of the storage method of operation in comparison with the resistance" misses ductivity of the photo-conducting nim M is changed by Bradiations, but is not elected by .li-radiations. In the case o! the photo-conducting hlm 4I, the reverse is true as its conductivity is changed by .lt-radiations, but is unailected by B-radiations. A-radiations reiiected by the object are projected through the conducting layer 46 onto the first nlm le and a beam of B- radiations passes through the conducting Layer and theiirstillmtoscanthe secondiilm, whereby a moving conductive path is provided between the conducting layer 40 and the metal plate Il, the external circuit is completed, and an image current, controlled by the variations in conductivity successively caused in small areas ox' the first nlm by .li-radiations, iiows through the external circuit. I! the second film N is made very thin and of high specific resistance when dark (that is, when not illuminated with the radiations to which it is sensitive), there is provided between the first illm Il and the metal plate il a capacity in which image impulses, corresponding to the elemental areas ot the image. may be stored and hence a greatly increased image current flow is produced in the external circuit, which circuit is similar to that shown in Fig. 1. if the A-radiations are red or infra-red, the photo-conducting iilm 45 may be selenium lor the resistance method or mercury iodide ior the storage method and a suitable photo-conducting nlm 44, sensitive to B-radiations (blue, violet, or ultra-violet), may consist of thallium bromide or chloride which may be used for either method as the specific resistance of the iilm M when illuminated does not have to be as high as thatoi theiilml asthisiilmuisusedtodischarge the stored charge rather than to store it up.

Fig. 4 shows a scanning tube S', which is adapted to be used in cases where the image is projected from a position in front of the target and a scanning beam is applied from a behind the target. Referring more particularly to Fig. 5, which is an enlarged perspective view oi the assembly within the tube Si, this tube comprises an evacuated container in which is mounted a composite target il, comprising a transparent supporting plate il of glass or similar material coated with a transparent metal layer 52 oi a suitable substance such as silver, iilms M and 45, and a transparent conducting layer It. The films and the conducting layer are similar to those described above with reference to Fig. 3. The external circuit is connected between the transparent metal layer l2 and the conducting layer le by a connection not shown in the drawmethod, and the relation of lateral to transverse conductivity in thin high resistance lms reference may be made to Patent 2,195,485, issued April 2, 1940 to Frank Gray. A suitable photoconducting material which is of suiiiciently high specific resistance to operate in accordance with the storage method and which is sensitive to red or infra-red radiations is mercurio iodide (Hgh) An enlarged perspective view of a modified scanning tube is shown in Fig. 3. 1in this embodiment there is no mesh electrode, the external circuit being connected between the metal plate Il and a light transmitting conducting layer on the target. The composite target 41 comprises the metal plate I3 carrying two photoconducting films M and li of diner-ent materials and a transparent conducting layer.` The eon- 7s ing. The scanning beam is produced by the iiuorescent screen of the cathode ray tube C, this and the optical systems Il and Il being similar to those disclosed in connection with Fig. 1. Image controlled radiations are projected through the transparent conducting layer Il onto the photo-conducting iilm li to ntrol its conductivity in accordance with the tone values of the object. The scanning beam B from the nuorescent screen or the cathode ray tube C passes through the transparent plate ll and the transparent conducting layer I! to scan successively the elemental areas oi.' he ting nlm u to impart conductivity to these elemental areas in succession. An image airrent is, therefore, produced which iiuws thimmh the external circuitinamannersimilartothatdelcribed above. 'Iiiistwillnlsooperatein accordance with the above.

Figs. 6, 7 and 8 each includes a target, similar to that disclosed with reference to Fig. except for the differences noted below in the description of each figure, mounted on the external surface of the end wall 60 of the scanning cathode ray tube C.

In Fig. 6, the end wall 60 takes the place of the glass plate 5i of Fig. 5, but the target is otherwise similar. It comprises a transparent metal layer 52, preferably of silver, two photo-conducting films 44 and 45 of different materials, respectively similar to the photo-conducting films described in connection with Fig. 3 and a conducting layer 46 of silver or the like. While the glass enclosure 6| for the target is shown attached to the end wall of the cathode ray tube C, it may be spaced therefrom and have the target mounted in a position intermediate the walls of the container 6|. This construction would include a glass plate similar to 5| of Fig. 5. The operation of the device shown in this figure is similar to that described above with reference to Fig. 4.

In Fig. 7, the two photo-conducting films are made of the same material and are separated by a medium to prevent radiations applied to one film from affecting the other film. The target thus comprises a transparent metallic layer 52, photo-conducting films 54 and 55, a thin, black, high resistance layer 56, made of Bakelite or similar material, placed between the two photoconducting films to prevent radiations applied to the film 55 from affecting film 54, and vice versa, and a conducting layer 46. With this construction, the same type of radiations may be used to both illuminate the image field and to scan the target. The method (or methods) of operation is similar to that of Fig. 6. The resistance layer 56 is so thin and of such high specific resistance that its lateral conductivity is small with respect to its transverse conductivity.

Fig. 8 shows a target in which a single film 62 is mounted between the conducting layers 52 and 46 and it is just thick enough to prevent both the scanning beam and the radiations applied to the image field from affecting it throughout. This design permits the use of the same type of radiations for both illuminating the field and scanning the target. The film 62, as well as the films 54 and 55 of Fig. 7, may be made of the same material as either film 44 or 45 of Fig. 3, depending on the type oi' radiations it is desired to use. The operation of the device shown in this figure is similar to that described above in connection with Fig. 7, the single thick film 62 of this figure performing the functions of both films 54 and 55 of Fig. 7. In this figure, as well as in Fig. 7, the glass enclosure 6I has been omitted but it is preferable to have such an enclosure to protect the thin lavers or films comprising the target.

In Figs. 6 to 8, inclusive. an optical system i9, similar to that shown in Fig. l, may be used for projecting radiations from Ithe image O on the target. It would also be satisfactory to use the same type of external circuit as-used in that figure. j

While this invention has been shown as applied to the situation where the object is a human being, it will be apparent that the invention is also applicable to the transmission of outdoor scenes or motion picture films, either using radiations reflected from the film. or passing through it, to control the operation of the scanning screen or target.

"storage method described radiations While several specific embodiments for utilizing the invention have been disclosed, it is to be understood that this invention is not limited thereto, but only by the scope of the appended claims. In these claims, the term sensitive to as used to describe certain elements is intended to include both photo-conducting and photo-emissive materials. The term light" in the claims is intended to include ultra-violet and infra-red radiations as well as radiations from the visible spectrum.

This application is a division of application Serial No. 67,059, filed March 4, 1936, by Frank Gray which was issued on March 14, 1939 as Patent 2,150,159. Application Serial No. 273,897, filed May 16, 1939, is a division of this application and is directed to system combinations disclosed herein, different from the system combinations claimed in said Patent 2,150,159; by system combinations being meant combinations involving elements both within and Without the closed Vessels, or tubes. shown in the drawings, the claims of the present application being directed to the tube structures disclosed.

What is claimed is:

1. An electro-optical device having a target adapted to have light radiations of one wavelength range applied thereto from an object and light radiations of a second wave-length'range applied thereto to scan it comprising a metal supporting plate having a face of relatively large area compared with the area of any of its edges, a layer of photo-conducting material contiguous to said face of said plate, and a layer of photosensitive material contiguous to the face of said photo-conducting layer remote from the metal plate, said photo-conducting layer being sensitive to light radiations from one of said wave-length ranges but substantially insensitive to radiations from the other of said wave-length ranges and said photo-sensitive layer being substantially insensitive to radiations from the wave-length range to which the photo-conducting layer is sensitive but sensitive to radiations from the wave-length range to which the photo-conducting layer is substantially insensitive.

2. An electro-optical device having a target adapted to have light radiations of one wavelength range applied thereto from an object and light radiations of a second wave-length range applied thereto to scan it comprising a metal supporting plate having a face of relatively large area compared with the area of any of its edges, a first layer of photo-conducting material contiguous to said face of said plate, and a second layer of photo-conducting material contiguous to the face of said first photo-conducting layer remote from the metal plate, said first photoconducting layer being sensitive to light radiations from one of said wave-length ranges but substantially insensitive to radiations from the other of said wave-length ranges and said second photo-conducting layer being substantially insensitive to radiations from the wave-length range to which the first photo-conducting layer is sensitive but sensitive to radiations from the wave-length range to which the first photo-conducting layer is substantially insensitive.

3. An electro-optical device having a target adapted to have light radiations of one wavelength range applied thereto from an object and light radiations of a second wave-length range applied thereto to scan it comprising a metal member having a face of relatively large area compared with the area of any of its edges, a

rst layer of photo-conducting material contiguous to said face of said member and a second layer of photo-conducting material contiguous to the face of said first photo-conducting layer remote from the metal member, said tlrst photoconducting layer being sensitive to light radiations from one of said wave-length ranges but substantially insensitive to radiations from the other of said wave-length ranges and said second photo-conducting layer being substantially insensitive to radiations from the wave-length range to which the first photo-conducting layer is sensitive but sensitive to radiations from the wave-length range to which the nrst photo-conducting layer is substantially insensitive.

4. An electro-optical device having a target adapted to have light radiations of one wavelength range applied thereto from an object and light radiations of a second wave-length range applied thereto to scan it comprising a metal supporting plate having a face of relatively large area compared with the area of any of its edges, a layer of photo-conducting material contiguous to said face of said plate and a layer of photoemissive material contiguous to the face oi said photo-ernissive layer remote from the metal plate, said photo-conducting layer being sensitive to light radiations from one of said wave-length ranges but substantially insensitive to radiations from the other of said wave-length ranges and said photo-emssive layer being substantially insensitive to radiations from the Wave-length range to which the photo-conducting layer is sensitive but sensitive to radiations from the wave-length range to which the photo-conducting layer is substantially insensitive.

5. An electro-optical device having a target adapted to have light radiations of one wavelength range applied thereto from an object and light radiations of a second Wave-length range applied thereto to scan it comprising a metal supporting plate having a face of relatively large area compared with the area of any of its edges, a layer of photo-conducting material contiguous to said face of said plate, a layer of photo-emissive material contiguous to the face of said photoemissive layer remote from the metal plate, said photo-conducting layer being sensitive to light radiations from one of said wave-length ranges but substantially insensitive to radiations from the other of said wave-length ranges and said photo-emissive layer being substantially insensitive to radiations from the wave-length range to which the photo-conducting layer is sensitive but sensitive to radiations from the wave-length range to which the photo-conducting layer is substantially insensitive, and a light permeable metallic member adjacent to said photo-emissive member but separated therefrom.

6. An electro-optical device having a' target adapted to have light radiations of one wavelength range applied thereto from an object and light radiations of a second wave-length range applied thereto to scan it comprising a metal supporting plate having a face of relatively large area. compared with the area of any of its edges, a layer of photo-conducting material contiguous to said face of said plate, and a layer of photosensitive material contiguous to the face of said photo-conducting layer remote from the metal plate, said photo-conducting layer being sensitive to light radiations from one of said wavelength ranges but substantially insensitiveto radiations from the other of said wave-length ranges and said photo-sensitive layer being substantially insensitive to radiations from the wave-length range to which the photo-conducting layer is sensitive but sensitive to radiations from the wave-length range to which the photo-conducting layer is substantially insensitive, said photo-sensitive layer being capable of transmitting to said photo-conductinl layer light to which the latter is responsive.

1. An electro-optical device having a target adapted to have light radiations of one wavelength range applied thereto from an object and light radiations of a second wave-length range applied thereto to scan it comprising a metal supporting plate having a face of relatively large area compared with the area of any of its edges, a iirst layer oi' photo-conducting material contiguous to said face of said plate and a second layer of photo-conducting material contiguous to the face oi' said iirst photo-conducting layer remote from the metal plate, said ilrst photo-conducting layer being sensitive to light radiations from one of said Wave-length ranges but substantially insensitive to radiations from the other of said wave-length ranges and said second photo-conducting layer being substantially insensitive to radiations from the wave-length range to which the first photo-conducting layer is sensitive but sensitive to radiations from the Wave-length range to which the first photo-conducting layer is substantially insensitive, at least one of said photo-conducting layers having a high specific resistance in the dark condition at least.

8. An electro-optical device having a target adapted to have light radiations of one wavelength range applied thereto from an object and light radiations of a second wave-length range applied thereto to scan it comprising a metal supporting plate having a face of relatively large area compared with the area ci any of its edges, a first layer o! photo-conducting material contiguous to said face of said plate and a second layer of photo-conducting material contiguous to the face of said iirst photo-conducting layer remote from the metal plate, said ilrst photoconducting layer being sensitive to light radiations from one of said wave-length ranges but substantially insensitive to radiations from the other of said wave-length ranges and said second photo-conducting layer being substantially insensitive to radiations from the wave-length range to which the first photo-conducting layer is sensitive but sensitive to radiations from the wave-length range to which the first photo-conducting layer is substantially insensitive, at least one of said photo-conducting layers having a high specic resistance in the dark condition at least and the other of said layers having a high specific resistance in both the light and dark conditions.

9. An electro-optical device having a target adapted to have light radiations of one wavelength range applied thereto from an object and light radiations oi a second wave-length range applied thereto to scan it comprising a metal supporting plate having a face of relatively large area compared with the area of any of its edges, a layer o! photo-conducting material contiguous to said face of saldi plate and a layer of photosensitive material contiguous to the face of said photo-conducting layer remote from the metal plate, said photo-conducting layer being sensitive to light radiations from one of said wave-length ranges but substantially insensitive to radiations from the other of said wave-length ranges and said photo-sensitive layer being substantially in-i sensitive to radiations from the wave-length range to which the photo-conducting layer is sensitive but sensitive to radiations from the wave-length range to which the photo-conducting layer is substantially insensitive, said photoconducting layer being of high specific resistance in both the light and dark conditions whereby electric charges may be stored thereacross.

10. An electro-optical device having a target adapted to have light radiations of one wavelength range applied thereto from an object and light radiations of a second wave-length range applied thereto to scan it comprising a transparent supporting plate having a face of relatively large area compared with the area of any of its edges, a light transmitting metallic member contiguous to said face of said plate, a layer of photo-conducting material contiguous to the face of said metallic member remote from said supporting plate, a second layer of photo-conducting material contiguous to the face of said first photo-conducting Amaterial remote from the metal member, said first photo-conducting layer being sensitive to light radiations from one of said wave-length ranges but substantially insensitive to radiations from the other of said wave-length ranges and said second photo-conducting'layer being substantially insensitive to radiations from the wave-length range to which the first photo-conducting layer is sensitive but sensitive to radiations from the wave-length range to which the first photo-conducting layer is substantially insensitive, and a. light transmitting metallic member' contiguous to the face of said second photo-conducting layer remote from said first photo-conducting layer.

11. An electro-optical device having a target adapted to have compared with the area of any of its edges, a first layer of photo-conducting material contiguous to said face of said member, a second layer of photo-conducting material contiguous to the surface of said rst photo-conducting layer remote from the metal member, said iirst photoconducting layer being sensitive to light radiations from one of said wave-length ranges but substantially insensitive to radiations from the other of said wave-length ranges and said second photo-conducting layer being substantially insensitive to radiations from the wavelength range to which the first photo-conducting layer is sensitive but sensitive to radiations from the wave-length range to which the first photoconducting layer is substantially insensitive, and a light transmitting metallic member contiguous to the face of said second photo-conducting layer remote from said first photo-conducting layer.

12. A target for a cathode ray device comprising a film of fiuorescent material having an extended surface, a transparent metallic film adjacent said extended surface of said fluorescent film, a member formed of photo-conducting material contiguous to the face of the metallic film remote from the fluorescent film, and a second metallic film contiguous to the face of the photo-conducting member remote from the first metallic film.

13. A target for a cathode ray device comprising a iilm of fiuorescent material having an extended surface, a transparent metallic film adjacent said extended surface of said fluorescent film, a first; photo-conducting layer contiguous to the face of the metalic film remote from the fiuorescent screen. a second photo-conducting layer contiguous to the face of lthe first `photoconducting layer remote from the metallic film, and a second metallic film contiguous to the face of the photo-conducting member remote from the first metallic film.

FRANK GRAY. 

